Presentation about How Superconductivity was discovered, Types and Properties of Superconductors and Applications of Superconductors.

1. Superconductivity - Introduction
• The research about superconductors began when
Kamerlingh Onnes found that the resistivity of Hg
suddenly dropped to zero at 4.2K (liquid He
Temperature).
• At very low temperatures normal conductors retain
some resistivity but the resistivity of
superconductors suddenly drop to zero .
• A normal conductor can be brought into
superconducting state by increasing it’s pressure.

2. Transition Temperature OR Critical Temperature
Temperature at which a
normal conductor loses its
resistivity and becomes a
superconductor.
• Definite for a material
• Superconducting transition
reversible
• Good electrical conductors
like Cu, Ag, Au are not
superconductors and good
superconducting materials
are not good electrical
conductors.
Resistance (Ω)
4.0 4.1 4.2 4.3 4.4
Temperature (K)
0.15
0.10
0.0
Tc

3. Occurrence of Superconductivity
Superconducting Elements TC (K)
Sn (Tin) 3.72
Hg (Mercury) 4.15
Pb (Lead) 7.19
Superconducting Compounds
NbTi (Niobium Titanium) 10
Nb3Sn (Niobium Tin) 18.1

4. Superconductivity -Properties
1. Electrical Resistence
• Zero electrical resistence
• Ratio of resistance of
material in
superconducting state to
the same material in
normal state is less then 10-
5 .
r
s
r
<10-5
n

5. Superconductivity -Properties
2. Effect of magnetic field
• When the superconducting materials are subjected to large value
of magnetic field, it’s superconducting property gets destroyed.
• Critical magnetic field (HC) – Minimum magnetic field required to
destroy the superconducting property at any temperature
é æ ö 2
ù
H H T
= ê - ç ¸ ú
0 1 C
T
êë è C
ø úû
H0 – Critical field at 0K
T - Temperature below TC
TC - Transition Temperature

6. Normal
Superconducting
T (K) TC
H0
HC
Element HC at 0K
(mT)
Nb 198
Pb 80.3
Sn 30.9
Magnetic field vs Temperature
Examples of critical fields of some
superconducting materials

7. Superconductivity -Properties
3. Effect of Electric Current
• The application of large value of electric current to a
superconducting material induces a magnetic field in the
material and thus destroys it’s superconducting property.
• Induced Critical Current iC = 2πrHC
where Hc is the critical magnetic field required and r is the
radius of superconductor .
i

8. Superconductivity -Properties
4. Effect of Entropy
6. Thermal Conductivity
5. Specific Heat
Temperature
Temperature
Temperature

9. 7. Diamagnetic property :- Meissner Effect
• Magnetic Lines of force penetrate through a normal conducting
material when placed in a magnetic field of flux density B.
• Whereas, a superconducting material repels the magnetic field &
thus behaves as a diamagnetic material.
• A superconducting material also ejects magnetic lines of force
when cooled for superconductivity.
B ¹0 B = 0
Normal state
T>Tc
H>Hc
Superconducting
state
T<Tc
H<Hc

10. Types of Superconductors
Type I
• Exhibit Meissner Effect
• Behave as a prefect diamagnetic
material
• There is only one Hc
• No mixed state is present
• Sudden loss of magnetisation
• Soft superconductor
• Eg. – Pb, Sn, Hg
Type II
• Does not exhibit complete
Meissner Effect
• Does not behave as a perfect
diamagnetic material
• There are two HCs – HC1 & HC2
• Mixed state present
• Gradual loss of magnetisation
• Hard superconductor
• Eg. – Nb-Sn, Nb-Ti
M
Superconducting
Normal
H H C
Super-conducting
-M
Normal
Mixed
HC1 HC
HC2
H

11. High-Temperature Superconductors
• High Temperature superconductors have high Tc values.
• They are not metal or intermetallic compounds but oxides of
copper in combination with other elements.
• In 1983, 1987 & 1988, materials with Tc up to 40K, 93K and 125K
have been discovered respevtively.
• The HTSC compounds are represented by simplified notations as
1212, 1234, etc. These notations are based on number of atoms in
each metal element.
• They are brittle and easy to form wires and tapes.
• HTSC wires/tapes provide transmission of electrical power over a
long distance without any resistive loss.

12. High-Temperature Superconductors

13. Application of Superconductors
1. Josephson Effect
• In 1962, Brain Josephson predicted the flow of current in
insulator sandwiched between two superconductors on the
application of a D.C. Voltage.
Insulator

14. Components Of Current
• D.C. Component of Current – This component of
current exists even after the applied voltage is
removed.
• A.C. Component of Current – This component of
current exists only during the existence of applied
voltage.
The frequency of A.C. components is
g = 2eV / h

15. Uses of Josephson devices
• Magnetic Sensors
• Gradiometers
• Oscilloscopes
• Decoders
• Analogue to Digital converters
• Oscillators
• Microwave amplifiers
• Sensors for biomedical, scientific and defence purposes
• Digital circuit development for Integrated circuits
• Microprocessors
• Random Access Memories (RAMs)

16. Application of Superconductors
2. SQUID
(Superconducting Quantum Interface Device)
• SQUID is a type of magnetometer.
• It is the most sensitive type of detector known to science.
• Low Temperature superconductors are used for fabricating SQUID.
• It consists of a superconducting loop of two Josephson junctions.

17. Discovery:
• The DC SQUID was invented in 1964 by Robert Jaklevic, John
Lambe, Arnold Silver and James Mercereau of Ford Research
Labs
Principle :
• Small change in magnetic field, produces variation in the flux
quantum.
Uses :
• Storage device for magnetic flux
• Study of earthquakes
• Removing paramagnetic impurities
• Detection of magnetic signals from brain, heart etc.

18. Application of Superconductors
i
A
B
3.Cryotron
The cryotron is a switch
that operates using
superconductivity. The
cryotron works on the
principle that magnetic
fields destroy
superconductivity.

19. • Hca & Hcb are critical fields of material A & B
respectively & Hca<Hcb.
• The current ‘i’ induces some magnetic field ‘H’
in both materials. If ‘H’ lies between Hca & Hcb,
then the induced field will destroy the
superconductivity of material A & hence
contact will be broken due to increase in
resistivity.

20. Application of Superconductors
4. Maglev (Magnetic Leviation)
• Principle: Electro-magnetic
induction
 Magnetic levitation transport,
or maglev, is a form of
transportation that suspends,
guides and propels vehicles via
electromagnetic force. This
method can be faster than
wheeled mass transit systems,
potentially reaching velocities
comparable to turboprop and jet
aircraft (500 to 580 km/h).

21. Advantages
 No need of initial energy in case of magnets for low speeds
 One litre of Liquid nitrogen costs less than one litre of mineral water
 Onboard magnets and large margin between rail and train enable highest
recorded train speeds (581 km/h) and heavy load capacity. Successful
operations using high temperature superconductors in its onboard magnets,
cooled with inexpensive liquid nitrogen
 Magnetic fields inside and outside the vehicle are insignificant; proven,
commercially available technology that can attain very high speeds (500
km/h); no wheels or secondary propulsion system needed
 Free of friction as it is “Levitating”